† Corresponding author. E-mail:
Project supported by the National Key Research and Development Program of China (Grant Nos. 2017YFB0403100 and 2017YFB0403101), the National Natural Science Foundation of China (Grant Nos. 61704149, 61674076, and 61605071), the Natural Science Foundation of Jiangsu Province, China (Grant Nos. BY2013077, BK20141320, and BE2015111), the Project of Science and Technology Development Program in Shandong Province, China (Grant Nos. 2013YD02054 and 2013YD02008), the Project of Shandong Provincial Higher Educational Science and Technology Program, China (Grant No. J13LN08), the Collaborative Innovation Center of Solid State Lighting and Energy-saving Electronics, Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD), the Six-Talent Peaks Project of Jiangsu Province, China (Grant No. XYDXX-081), the Open Fund of the State Key Laboratory on Integrated Optoelectronics, China (Grant No. IOSKL2017KF03), the Project of Autonomous Innovation and Achievement Transformation Program in Zaozhuang City, China (Grant No. 2017GH3), the Overseas Study Program Funded by Shandong Provincial Government, China, the Laboratory Open Fund from Jiangsu Key Laboratory of Photoelectric Information Functional Materials, China, and the Doctoral Foundation Project of Zaozhuang University, China.
The Mg acceptor activation mechanism and hole transport characteristics in AlGaN alloy with Mg doping concentration (∼ 1020 cm−3) grown by metal–organic chemical vapor deposition (MOCVD) are systematically studied through optical and electrical properties. Emission lines of shallow oxygen donors and (VIII complex)1− as well as
Aluminum–gallium–nitride (AlGaN) alloy is recognized as one of most promising materials for applications in deep ultraviolet (DUV) light emitting diode (LED) devices,[1–3] due to their great potential applications in sterilization, water purification, and biological and chemical agent detection.[4,5] In order to fabricate high efficiency DUV-LEDs, it is required to obtain a highly conductive p-type AlGaN layer with a high AlN mole fraction. However, since the ionization energy for Mg-doped AlxGa1 − xN alloys dramatically increases with AlN mole fraction increasing from 170 meV (for x = 0) to 630 meV (for x = 1),[6,7] which leads to very small hole concentration in the valence band at room-temperature. Therefore it is rather difficult to achieve highly conductive p-type AlGaN.
Recently, very high Mg-doped level (around 1020 cm−3–1021 cm−3) could be adopted to obtain adequate free hole conductivity, because of the low activation ratio of holes in AlGaN with high AlN mole fraction.[8] But high doping effect easily leads to the valence band-tail states and impurity band to form.[9] In addition, since the formation energy values of intrinsic defects and their complexes are significantly reduced in highly p-type Al-rich AlGaN alloys, these defects could further compensate for the presence of free holes.[10,11] So the fundamental understanding of the impurity transitions, as well as Mg acceptor activation mechanism and hole transport characteristics in highly Mg-doped AlGaN has become increasingly important.
In this paper, we systematically investigate the optical transitions of impurity transitions and variable-temperature Hall effect to clarify the Mg acceptor activation mechanism and transport characteristics in highly Mg-doped AlGaN alloys. The optical characteristics of undoped AlGaN and Mg-doped AlGaN alloys are investigated by using the cathodoluminescence (CL). The electrical properties of each sample are analyzed by using the temperature-dependent Hall effect measurements. It is discovered that there exists a pronounced reduction activation energy for Mg acceptor and lower hole mobility in highly Mg-doped AlGaN alloys, due to the high ionized acceptor concentration and compensation ratio.
The unintentionally doped and Mg-doped AlGaN alloys were grown by metal–organic chemical vapor deposition (MOCVD) using trimethylaluminum (TMAl), trimethylgallium (TMGa), ammonia (NH3) as the organometallic precursors for Al, Ga, and N, respectively. Hydrogen (H2) was used as the carrier gas. For Mg doping, an optimized molar flux of biscyclopentadienyl-magnessium (Cp2Mg) at 4.8 × 10−7 mol/min was used. More detailed growth procedures for undoped and Mg-doped AlxGa1 − xN alloys were reported in Refs. [12,13]. The AlN mole fractions of AlGaN samples were determined by high-resolution x-ray diffraction (HRXRD) through using Cu K line = 0.15406 nm radiation (PANalytical X’Pert Pro XRD). The concentration of Mg atoms incorporated into Mg-doped AlGaN alloys was determined to be 1 × 1020 cm−3 by using secondary ion mass spectrometry (SIMS).[13] The optical properties were characterized by cathodo-luminescence spectra (CL, Gatan Mono CL3+) at low temperature ∼ 120 K. Post growth rapid thermal annealing in N2 ambient was used to activate Mg acceptor. The electrical properties were measured by variable-temperature Hall effect measurement through using the van der Pauw method (Accent HL5500 measurement system).
Figure
Figure
![]() | Fig. 2. (a) CL peak position (Eemi) of present impurity transition (solid stars) observed from Fig. |
To obtain a more comprehensive picture of O donor and (VIII-complex)−1 acceptor energy levels in undoped AlGaN alloy, we plot its donor, acceptor energy levels, conduction (Ec), and valence (Ev) band edges versus AlN mole fraction x in Fig.
For Mg-doped AlGaN alloys, the band edge transitions become completely quenched asindicated by the solid line of Fig.
![]() | Fig. 3. Plots of energy levels (EA, ED) of acceptor and donor with conduction and valence band edge (Ec, Ev) versus AlN mole fraction (x) in Mg-doped AlxGa1 − xN alloys. |
In order to characterize the ionization of Mg acceptor, we carry out the temperature-dependent Hall effect measurements. The resistivity for Mg-doped Al0.57Ga0.43N alloy is highly resistive (not shown), which is most likely to be due to the resistivity exponentially increasing with the activation energy (EA), and being compensated for by nitrogen vacancies (as shown in Fig.
Since the resistivity includes the contributions from both hole concentration (p) and mobility (μ), we evaluate the EA values of Mg acceptors for Mg-doped AlxGa1 − xN (x = 0.23 and 0.35) based on the temperature-dependent free hole concentration as shown in Fig.
For the Mg-doped Al0.35Ga0.65N alloys, the hole concentration also increases with temperature increasing due to the thermal ionization of Mg dopants. There exists a deviation between the experimental measurement data and the fitting curve at temperatures ranging from 260 K to 360 K, which implies that the thermal activation of holes starts to play a role. But only temperature above 360 K, the thermal activation becomes dominant for the hole transport mechanism. The fitting lines are obtained by the following Eqs. (
![](cpb_29_5_058103/cpb_29_5_058103_ieqn6.gif)
![]() | Table 1. Fitting results from variable Hall measurements of the Mg-doped AlxGa1 − xN (x = 0.23 and 0.35) alloys. . |
The values of activation energy (EA) are 172 meV and 242 meV for Mg-doped Al0.23Ga0.77N, and Al0.35Ga0.65N, respectively, which are lower than the previously estimated value of of EA as a function of the AlN mole fraction in Mg-doped AlGaN alloys.[6] The lowering of the value of the activation energy (ΔEA) is ascribed to the combined effect of the Coulomb potentials of the Mg dopants and the screening of the Coulomb potentials by a high concentration of free holes. Moreover, ΔEA is assumed to be proportional to the average distance
Thus, the acceptor activation energy may be expressed as
In this work, the optical and electrical characteristics of highly Mg-doped AlxGa1 − xN alloys (0.23 ≤ x ≤ 0.57) are investigated. Their cathodo-luminescence spectra show that there exist two groups of impurity transitions in Mg-doped AlGaN alloys: one is assigned to the recombination between electrons bound to shallow oxygen donors and (VIII-complex)1−, and the other is the recombination of electrons bound between
[1] | |
[2] | |
[3] | |
[4] | |
[5] | |
[6] | |
[7] | |
[8] | |
[9] | |
[10] | |
[11] | |
[12] | |
[13] | |
[14] | |
[15] | |
[16] | |
[17] | |
[18] | |
[19] | |
[20] | |
[21] | |
[22] | |
[23] | |
[24] | |
[25] | |
[26] | |
[27] | |
[28] | |
[29] | |
[30] | |
[31] | |
[32] | |
[33] | |
[34] | |
[35] |